US20250056858A1 - Group iii-nitride semiconductor structure on silicon-on-insulator and method of growing thereof - Google Patents
Group iii-nitride semiconductor structure on silicon-on-insulator and method of growing thereof Download PDFInfo
- Publication number
- US20250056858A1 US20250056858A1 US18/720,416 US202218720416A US2025056858A1 US 20250056858 A1 US20250056858 A1 US 20250056858A1 US 202218720416 A US202218720416 A US 202218720416A US 2025056858 A1 US2025056858 A1 US 2025056858A1
- Authority
- US
- United States
- Prior art keywords
- layer
- silicon
- iii
- active
- epitaxial
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Pending
Links
- 239000012212 insulator Substances 0.000 title claims abstract description 115
- 239000004065 semiconductor Substances 0.000 title claims abstract description 93
- 238000000034 method Methods 0.000 title claims description 22
- 239000000758 substrate Substances 0.000 claims abstract description 121
- 229910052710 silicon Inorganic materials 0.000 claims abstract description 112
- 239000010703 silicon Substances 0.000 claims abstract description 112
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 claims abstract description 111
- 230000005533 two-dimensional electron gas Effects 0.000 claims abstract description 10
- 229910002601 GaN Inorganic materials 0.000 claims description 39
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 claims description 34
- JMASRVWKEDWRBT-UHFFFAOYSA-N Gallium nitride Chemical compound [Ga]#N JMASRVWKEDWRBT-UHFFFAOYSA-N 0.000 claims description 28
- 238000009792 diffusion process Methods 0.000 claims description 25
- 239000002019 doping agent Substances 0.000 claims description 23
- HBMJWWWQQXIZIP-UHFFFAOYSA-N silicon carbide Chemical compound [Si+]#[C-] HBMJWWWQQXIZIP-UHFFFAOYSA-N 0.000 claims description 19
- 125000006850 spacer group Chemical group 0.000 claims description 18
- 239000000377 silicon dioxide Substances 0.000 claims description 15
- 229910021417 amorphous silicon Inorganic materials 0.000 claims description 14
- 235000012239 silicon dioxide Nutrition 0.000 claims description 13
- 238000004519 manufacturing process Methods 0.000 claims description 12
- 229910052581 Si3N4 Inorganic materials 0.000 claims description 9
- HQVNEWCFYHHQES-UHFFFAOYSA-N silicon nitride Chemical compound N12[Si]34N5[Si]62N3[Si]51N64 HQVNEWCFYHHQES-UHFFFAOYSA-N 0.000 claims description 9
- RNQKDQAVIXDKAG-UHFFFAOYSA-N aluminum gallium Chemical compound [Al].[Ga] RNQKDQAVIXDKAG-UHFFFAOYSA-N 0.000 claims description 6
- 229910052785 arsenic Inorganic materials 0.000 claims description 5
- 229910052698 phosphorus Inorganic materials 0.000 claims description 5
- PMHQVHHXPFUNSP-UHFFFAOYSA-M copper(1+);methylsulfanylmethane;bromide Chemical compound Br[Cu].CSC PMHQVHHXPFUNSP-UHFFFAOYSA-M 0.000 claims description 4
- 229910052814 silicon oxide Inorganic materials 0.000 claims description 4
- 229910052787 antimony Inorganic materials 0.000 claims description 3
- OAICVXFJPJFONN-UHFFFAOYSA-N Phosphorus Chemical compound [P] OAICVXFJPJFONN-UHFFFAOYSA-N 0.000 claims description 2
- WATWJIUSRGPENY-UHFFFAOYSA-N antimony atom Chemical compound [Sb] WATWJIUSRGPENY-UHFFFAOYSA-N 0.000 claims description 2
- RQNWIZPPADIBDY-UHFFFAOYSA-N arsenic atom Chemical compound [As] RQNWIZPPADIBDY-UHFFFAOYSA-N 0.000 claims description 2
- 238000005468 ion implantation Methods 0.000 claims description 2
- 239000011574 phosphorus Substances 0.000 claims description 2
- 239000010410 layer Substances 0.000 description 365
- 238000002161 passivation Methods 0.000 description 18
- 230000005012 migration Effects 0.000 description 16
- 238000013508 migration Methods 0.000 description 16
- 239000012535 impurity Substances 0.000 description 15
- 230000007480 spreading Effects 0.000 description 10
- 238000003892 spreading Methods 0.000 description 10
- 238000005259 measurement Methods 0.000 description 9
- 229910052782 aluminium Inorganic materials 0.000 description 8
- 229910052733 gallium Inorganic materials 0.000 description 8
- 230000010287 polarization Effects 0.000 description 8
- 229910002704 AlGaN Inorganic materials 0.000 description 6
- 230000006870 function Effects 0.000 description 6
- 229910052757 nitrogen Inorganic materials 0.000 description 6
- 230000003287 optical effect Effects 0.000 description 6
- 229910021420 polycrystalline silicon Inorganic materials 0.000 description 6
- -1 for example Chemical class 0.000 description 5
- 229910052738 indium Inorganic materials 0.000 description 5
- 229920005591 polysilicon Polymers 0.000 description 5
- 230000008569 process Effects 0.000 description 5
- 229910010271 silicon carbide Inorganic materials 0.000 description 5
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 4
- GYHNNYVSQQEPJS-UHFFFAOYSA-N Gallium Chemical compound [Ga] GYHNNYVSQQEPJS-UHFFFAOYSA-N 0.000 description 4
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 4
- 229910052796 boron Inorganic materials 0.000 description 4
- 238000002955 isolation Methods 0.000 description 4
- 239000000203 mixture Substances 0.000 description 4
- QGZKDVFQNNGYKY-UHFFFAOYSA-N Ammonia Chemical compound N QGZKDVFQNNGYKY-UHFFFAOYSA-N 0.000 description 3
- 238000004871 chemical beam epitaxy Methods 0.000 description 3
- 238000005229 chemical vapour deposition Methods 0.000 description 3
- 230000008878 coupling Effects 0.000 description 3
- 238000010168 coupling process Methods 0.000 description 3
- 238000005859 coupling reaction Methods 0.000 description 3
- 238000000151 deposition Methods 0.000 description 3
- 238000005516 engineering process Methods 0.000 description 3
- 238000002513 implantation Methods 0.000 description 3
- 238000011065 in-situ storage Methods 0.000 description 3
- 239000000463 material Substances 0.000 description 3
- 238000001451 molecular beam epitaxy Methods 0.000 description 3
- 229910021421 monocrystalline silicon Inorganic materials 0.000 description 3
- 230000003071 parasitic effect Effects 0.000 description 3
- BLRPTPMANUNPDV-UHFFFAOYSA-N Silane Chemical compound [SiH4] BLRPTPMANUNPDV-UHFFFAOYSA-N 0.000 description 2
- 238000000231 atomic layer deposition Methods 0.000 description 2
- 239000000969 carrier Substances 0.000 description 2
- 238000005253 cladding Methods 0.000 description 2
- 150000001875 compounds Chemical class 0.000 description 2
- 230000008021 deposition Effects 0.000 description 2
- 230000000694 effects Effects 0.000 description 2
- APFVFJFRJDLVQX-UHFFFAOYSA-N indium atom Chemical compound [In] APFVFJFRJDLVQX-UHFFFAOYSA-N 0.000 description 2
- 230000010354 integration Effects 0.000 description 2
- 238000005240 physical vapour deposition Methods 0.000 description 2
- 230000009467 reduction Effects 0.000 description 2
- 238000004904 shortening Methods 0.000 description 2
- 229910052716 thallium Inorganic materials 0.000 description 2
- IBEFSUTVZWZJEL-UHFFFAOYSA-N trimethylindium Chemical compound C[In](C)C IBEFSUTVZWZJEL-UHFFFAOYSA-N 0.000 description 2
- ZOXJGFHDIHLPTG-UHFFFAOYSA-N Boron Chemical compound [B] ZOXJGFHDIHLPTG-UHFFFAOYSA-N 0.000 description 1
- 229910003828 SiH3 Inorganic materials 0.000 description 1
- 229910052768 actinide Inorganic materials 0.000 description 1
- 150000001255 actinides Chemical class 0.000 description 1
- 229910021529 ammonia Inorganic materials 0.000 description 1
- QVGXLLKOCUKJST-UHFFFAOYSA-N atomic oxygen Chemical compound [O] QVGXLLKOCUKJST-UHFFFAOYSA-N 0.000 description 1
- 230000004888 barrier function Effects 0.000 description 1
- 230000008901 benefit Effects 0.000 description 1
- 230000015572 biosynthetic process Effects 0.000 description 1
- 229910052797 bismuth Inorganic materials 0.000 description 1
- 230000000903 blocking effect Effects 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 230000008859 change Effects 0.000 description 1
- 229910021419 crystalline silicon Inorganic materials 0.000 description 1
- 230000007423 decrease Effects 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 230000002542 deteriorative effect Effects 0.000 description 1
- PZPGRFITIJYNEJ-UHFFFAOYSA-N disilane Chemical compound [SiH3][SiH3] PZPGRFITIJYNEJ-UHFFFAOYSA-N 0.000 description 1
- 230000005684 electric field Effects 0.000 description 1
- 238000000407 epitaxy Methods 0.000 description 1
- 238000011066 ex-situ storage Methods 0.000 description 1
- 230000005669 field effect Effects 0.000 description 1
- 239000007789 gas Substances 0.000 description 1
- 229910021478 group 5 element Inorganic materials 0.000 description 1
- 230000006872 improvement Effects 0.000 description 1
- 229910052747 lanthanoid Inorganic materials 0.000 description 1
- 150000002602 lanthanoids Chemical class 0.000 description 1
- 238000004377 microelectronic Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 229910000069 nitrogen hydride Inorganic materials 0.000 description 1
- 230000006911 nucleation Effects 0.000 description 1
- 238000010899 nucleation Methods 0.000 description 1
- 239000001301 oxygen Substances 0.000 description 1
- 229910052760 oxygen Inorganic materials 0.000 description 1
- 230000000737 periodic effect Effects 0.000 description 1
- 239000012071 phase Substances 0.000 description 1
- 239000002243 precursor Substances 0.000 description 1
- 238000012545 processing Methods 0.000 description 1
- 229910052706 scandium Inorganic materials 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
- 229910000077 silane Inorganic materials 0.000 description 1
- OLRJXMHANKMLTD-UHFFFAOYSA-N silyl Chemical compound [SiH3] OLRJXMHANKMLTD-UHFFFAOYSA-N 0.000 description 1
- 239000002356 single layer Substances 0.000 description 1
- 230000002269 spontaneous effect Effects 0.000 description 1
- 239000000126 substance Substances 0.000 description 1
- 230000005641 tunneling Effects 0.000 description 1
- 239000012808 vapor phase Substances 0.000 description 1
- 238000000927 vapour-phase epitaxy Methods 0.000 description 1
- 229910052727 yttrium Inorganic materials 0.000 description 1
Images
Classifications
-
- H01L29/2003—
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02002—Preparing wafers
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02367—Substrates
- H01L21/0237—Materials
- H01L21/02373—Group 14 semiconducting materials
- H01L21/02381—Silicon, silicon germanium, germanium
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02436—Intermediate layers between substrates and deposited layers
- H01L21/02439—Materials
- H01L21/02441—Group 14 semiconducting materials
- H01L21/0245—Silicon, silicon germanium, germanium
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02436—Intermediate layers between substrates and deposited layers
- H01L21/02439—Materials
- H01L21/02455—Group 13/15 materials
- H01L21/02458—Nitrides
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02436—Intermediate layers between substrates and deposited layers
- H01L21/02439—Materials
- H01L21/02488—Insulating materials
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02436—Intermediate layers between substrates and deposited layers
- H01L21/02494—Structure
- H01L21/02496—Layer structure
- H01L21/02505—Layer structure consisting of more than two layers
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02436—Intermediate layers between substrates and deposited layers
- H01L21/02494—Structure
- H01L21/02513—Microstructure
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02518—Deposited layers
- H01L21/02521—Materials
- H01L21/02538—Group 13/15 materials
- H01L21/0254—Nitrides
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/02104—Forming layers
- H01L21/02365—Forming inorganic semiconducting materials on a substrate
- H01L21/02612—Formation types
- H01L21/02617—Deposition types
- H01L21/0262—Reduction or decomposition of gaseous compounds, e.g. CVD
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/04—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
- H01L21/18—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
- H01L21/28—Manufacture of electrodes on semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/268
- H01L21/28008—Making conductor-insulator-semiconductor electrodes
- H01L21/28264—Making conductor-insulator-semiconductor electrodes the insulator being formed after the semiconductor body, the semiconductor being a III-V compound
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/04—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
- H01L21/18—Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
- H01L21/30—Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26
- H01L21/322—Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26 to modify their internal properties, e.g. to produce internal imperfections
- H01L21/3221—Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26 to modify their internal properties, e.g. to produce internal imperfections of silicon bodies, e.g. for gettering
- H01L21/3226—Treatment of semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/26 to modify their internal properties, e.g. to produce internal imperfections of silicon bodies, e.g. for gettering of silicon on insulator
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/70—Manufacture or treatment of devices consisting of a plurality of solid state components formed in or on a common substrate or of parts thereof; Manufacture of integrated circuit devices or of parts thereof
- H01L21/71—Manufacture of specific parts of devices defined in group H01L21/70
- H01L21/76—Making of isolation regions between components
- H01L21/762—Dielectric regions, e.g. EPIC dielectric isolation, LOCOS; Trench refilling techniques, SOI technology, use of channel stoppers
- H01L21/7624—Dielectric regions, e.g. EPIC dielectric isolation, LOCOS; Trench refilling techniques, SOI technology, use of channel stoppers using semiconductor on insulator [SOI] technology
- H01L21/76243—Dielectric regions, e.g. EPIC dielectric isolation, LOCOS; Trench refilling techniques, SOI technology, use of channel stoppers using semiconductor on insulator [SOI] technology using silicon implanted buried insulating layers, e.g. oxide layers, i.e. SIMOX techniques
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/70—Manufacture or treatment of devices consisting of a plurality of solid state components formed in or on a common substrate or of parts thereof; Manufacture of integrated circuit devices or of parts thereof
- H01L21/71—Manufacture of specific parts of devices defined in group H01L21/70
- H01L21/76—Making of isolation regions between components
- H01L21/762—Dielectric regions, e.g. EPIC dielectric isolation, LOCOS; Trench refilling techniques, SOI technology, use of channel stoppers
- H01L21/7624—Dielectric regions, e.g. EPIC dielectric isolation, LOCOS; Trench refilling techniques, SOI technology, use of channel stoppers using semiconductor on insulator [SOI] technology
- H01L21/76251—Dielectric regions, e.g. EPIC dielectric isolation, LOCOS; Trench refilling techniques, SOI technology, use of channel stoppers using semiconductor on insulator [SOI] technology using bonding techniques
-
- H01L29/66462—
-
- H01L29/778—
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/01—Manufacture or treatment
- H10D30/015—Manufacture or treatment of FETs having heterojunction interface channels or heterojunction gate electrodes, e.g. HEMT
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/40—FETs having zero-dimensional [0D], one-dimensional [1D] or two-dimensional [2D] charge carrier gas channels
- H10D30/47—FETs having zero-dimensional [0D], one-dimensional [1D] or two-dimensional [2D] charge carrier gas channels having 2D charge carrier gas channels, e.g. nanoribbon FETs or high electron mobility transistors [HEMT]
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D30/00—Field-effect transistors [FET]
- H10D30/40—FETs having zero-dimensional [0D], one-dimensional [1D] or two-dimensional [2D] charge carrier gas channels
- H10D30/47—FETs having zero-dimensional [0D], one-dimensional [1D] or two-dimensional [2D] charge carrier gas channels having 2D charge carrier gas channels, e.g. nanoribbon FETs or high electron mobility transistors [HEMT]
- H10D30/471—High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT]
- H10D30/475—High electron mobility transistors [HEMT] or high hole mobility transistors [HHMT] having wider bandgap layer formed on top of lower bandgap active layer, e.g. undoped barrier HEMTs such as i-AlGaN/GaN HEMTs
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D62/00—Semiconductor bodies, or regions thereof, of devices having potential barriers
- H10D62/80—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials
- H10D62/85—Semiconductor bodies, or regions thereof, of devices having potential barriers characterised by the materials being Group III-V materials, e.g. GaAs
- H10D62/8503—Nitride Group III-V materials, e.g. AlN or GaN
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10D—INORGANIC ELECTRIC SEMICONDUCTOR DEVICES
- H10D64/00—Electrodes of devices having potential barriers
- H10D64/60—Electrodes characterised by their materials
- H10D64/66—Electrodes having a conductor capacitively coupled to a semiconductor by an insulator, e.g. MIS electrodes
- H10D64/68—Electrodes having a conductor capacitively coupled to a semiconductor by an insulator, e.g. MIS electrodes characterised by the insulator, e.g. by the gate insulator
- H10D64/693—Electrodes having a conductor capacitively coupled to a semiconductor by an insulator, e.g. MIS electrodes characterised by the insulator, e.g. by the gate insulator the insulator comprising nitrogen, e.g. nitrides, oxynitrides or nitrogen-doped materials
Definitions
- the present disclosure generally relates, amongst others, to a semiconductor structure and to a method of growing thereof. More particularly, it relates to a semiconductor structure comprising Group III-nitride grown onto Silicon-On-Insulator, wherein the semiconductor structure achieves outstanding performance for high-power and high-frequency applications, and to a method of growing thereof.
- Group III-nitride-based heterostructures are very suited for high-power and high-frequency applications due to their high electron velocity and high critical electric field.
- AlGaN/GaN heterostructures are conventionally used for the manufacturing of field effect transistors also called FETs.
- FETs field effect transistors
- a two dimensional electron gas also referred to as 2DEG, is generated by the spontaneous and piezoelectric polarization between the two active layers, i.e., between AlGaN and GaN.
- Group III-nitride-based heterostructures are typically manufactured on top of conventional silicon substrates. With the ever increasing need for high-power and high-frequency solutions, the telecommunication industry is faced with the challenge of making such Group III-nitride-based heterostructures compatible with existing technologies. For example, Group III-nitride-based heterostructures should allow the continued miniaturization of microelectronic devices and the continued improvement of their performance.
- measurements performed with spreading resistance profiling on Group III-nitride heterostructures epitaxially grown on a silicon substrate demonstrate a similar drop in resistivity at the interface between the Group III-nitride heterostructure and the silicon substrate and similar presence of p-type dopants at the interface between the Group III-nitride heterostructure and the silicon substrate.
- Such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of impurities from the initial growth layer of the epitaxial layers of the Group III-nitride heterostructure to the silicon substrate.
- the impurities act as a p-type impurity for the silicon substrate.
- such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of Group III elements into the silicon substrate in which they act as p-type impurities for the silicon substrate.
- such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of gallium and/or aluminum into the silicon substrate.
- Gallium and/or aluminum act as p-type impurities for silicon and thereby change the resistivity of the silicon substrate.
- a semiconductor structure comprising:
- presence of p-type dopants at the interface between the Group III-nitride heterostructure and a silicon substrate onto which the Group III-nitride heterostructure is, for example, epitaxially grown can be measured with, for example, spreading resistance profiling measurements.
- Such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of impurities from the initial growth layer of the epitaxial layers of the Group III-nitride heterostructure to the silicon substrate.
- the impurities act as a p-type impurity for the silicon substrate. More particularly, such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of Group III elements into the silicon substrate in which they act as p-type impurities for the silicon substrate.
- the diffusion or migration of Group III elements from the epitaxial layers of the Group III-nitride heterostructure into the Silicon-On-Insulator substrate is contained in a surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure, for example, in the top layer and optionally close to the interface between the intermediate layer and the top layer.
- the intermediate layer of the Silicon-On-Insulator substrate confines the diffusion or migration of Group III elements within the surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure, for example, in the top layer and optionally close to the interface between the intermediate layer and the top layer, thereby shortening the diffusion distance of the impurities into the Silicon-On-Insulator substrate.
- the n-type doping of the top layer of the Silicon-On-Insulator substrate compensates for the concentration of Group III elements that diffuses from the epitaxial layers into the Silicon-On-Insulator substrate.
- the n-type doping of the top layer of the Silicon-On-Insulator substrate according to the present disclosure balances out a concentration of p-type dopants at the interface between the epitaxial layers and the Silicon-On-Insulator substrate, wherein the concentration of these p-type dopants results from a diffusion of Group III atoms from the epitaxial III-N semiconductor layer stack into the top layer of the Silicon-On-Insulator substrate.
- the semiconductor structure according to the present disclosure demonstrates improved performance at high-power and high-frequency, improved resistivity, and reduced power losses and linearity problems.
- trap-rich layer has been proven as one of the most effective techniques to reduce these parasitic effects and to enhance the high-resistivity properties of silicon, while being compatible with industrial SOI wafer fabrication and with the important thermal budget of standard CMOS process.
- the traps of the trap-rich layer capture the free carriers at the interface between the silicon and the intermediate layer, thereby enabling the Silicon-On-Insulator substrate to recover its nominal resistivity, linearity, eliminating the DC dependency and leading to a substantial reduction of RF losses and crosstalk.
- the trap-rich layer has a defect density suitable for trapping free charges that may be generated in the Silicon-On-Insulator substrate.
- the trap-rich layer may provide a trapping effect as well.
- the trap-rich layer has a thickness of several tens of nanometers to several microns, for example, 50 nm to 3 microns.
- the trap-rich layer comprises silicon, or amorphous silicon carbide, or polycrystalline silicon also referred to as polysilicon.
- a two-dimensional electron gas also referred to as 2DEG
- 2DEG is a gas of electrons free to move in two dimensions, but tightly confined in the first. This tight confinement leads to quantized energy levels for motion in that direction.
- the electrons appear to be a 2D sheet embedded in a 3D world.
- Group III-nitride refers to semiconductor compounds formed between elements in Group III of the periodic table, for example, Boron, also referred to as B, Aluminum, also referred to as Al, Gallium, also referred to as Ga, Indium, also referred to as In, and Nitrogen, also referred to as N.
- Example of binary Group III-nitride compounds are GaN, AIN, BN, etc.
- Group III-nitride also refers to ternary and quaternary compounds such as, for example, AlGaN and InAlGaN.
- the first active III-N layer comprises one or more of N, P, As, and one or more of B, Al, Ga, In and Tl.
- the first active III-N layer for example, comprises GaN.
- the second active III-N layer comprises one or more of N, P, As, and one or more of B, Al, Ga, In, and Tl.
- the second active III-N layer for example, comprises AlGaN.
- AlGaN relates to a composition comprising Al, Ga and N in any stoichiometric ratio (Al x Ga y N) wherein x is between 0 and 1 and y is between 0 and 1.
- the second active III-N layer for example, comprises AIN.
- the second active III-N layer comprises InAlGaN.
- a composition such as InAlGaN comprises In in any suitable amount.
- both first active III-N layer and second active III-N layer comprise InAlGaN, and the second active III-N layer comprises a bandgap larger than a bandgap of the first active III-N layer and wherein the second active III-N layer comprises a polarization larger than the polarization of the first active III-N layer.
- both first active III-N layer and second active III-N layer comprise BInAlGaN
- the second active III-N layer comprises a bandgap larger than a bandgap of the first active III-N layer and wherein the second active III-N layer comprises a polarization larger than the polarization of the first active III-N layer.
- Compositions of the active layer may be chosen in view of characteristics to be obtained, and compositions may vary accordingly. For example, good results were obtained with a first active III-N layer comprising GaN of about 150 nm thickness and a second active III-N layer comprising AlGaN of about 20 nm thickness.
- the base layer of the Silicon-On-Insulator substrate comprises bulk silicon and a resistivity of the base layer of the Silicon-On-Insulator substrate is typically between 3 and 5 kOhm ⁇ cm, and is preferably higher than 1 kOhm ⁇ cm. This way, the resistivity of the substrate underlying the epitaxial III-N semiconductor layer stack is maximized for high-power and high-frequency applications.
- Silicon-On-Insulator also referred to as SOI
- SOI Silicon-On-Insulator
- the choice of insulator depends largely on the intended application of the semiconductor devices.
- Several types of Silicon-On-Insulator substrates may be used within the context of the present disclosure.
- the semiconductor devices manufactured on Silicon-On-Insulator Due to the isolation from the bulk silicon of the base layer of the Silicon-On-Insulator substrate, parasitic capacitance within the semiconductor devices manufactured from the Group III-nitride heterostructure is lowered, thereby improving their power consumption and their performance.
- the semiconductor devices manufactured on Silicon-On-Insulator also demonstrate a higher resistance to latchup and a higher performance at equivalent VDD than semiconductor devices integrated on other types of substrates.
- the temperature dependency of the semiconductor devices manufactured on SOI is reduced compared to semiconductor devices integrated on other types of substrates. Due to the isolation, the semiconductor devices manufactured on SOI demonstrate lower leakage currents and consequently higher power efficiency.
- Radio-Frequency Silicon-On-Insulator substrates also referred to as RF-SOI substrates, enable high RF performance on silicon films compatible with standard CMOS processes, high linearity RF isolation and power signals, low RF loss, digital processing and power management integration.
- an enhanced signal integrity substrate for RF application comprises a base layer comprising high-resistive silicon, a trap rich layer formed on top of the base layer, a buried insulator formed on top of the trap rich layer, and a top layer formed on top of the buried insulator, wherein the top layer comprises a monocrystal.
- a resistivity of the base layer is typically over 3 kOhm ⁇ cm.
- a thickness of the top layer is typically between 50 nm and 200 nm.
- the addition of a trap-rich layer provides outstanding RF performances.
- Such substrate is particularly suited for devices with stringent linearity specifications. Applications typically target, for example, LTE-Advanced and 5G specifications and address different performance requirements.
- an enhanced signal integrity substrate Compared to a high-resistive SOI substrate, an enhanced signal integrity substrate demonstrates better linearity, lower RF losses, lower crosstalk, improved quality factors for passives, smaller die sizes and higher thermal conductivity. Enhanced signal integrity substrates further typically demonstrate a harmonic quality factor lower than ⁇ 80 dBm.
- a RF-SOI comprises a base layer comprising mid-resistive silicon, a trap-rich layer formed on top of the base layer, a buried insulator formed on top of the trap-rich layer, and a top layer comprising a thin monocrystal.
- Such substrate is particularly suited for, for example, cost sensitive highly integrated devices, and is particularly well suited to, for example, WI-FI®, IoT and other consumer applications specifications.
- Such substrate comprises a base layer comprising high-resistive silicon, a buried insulator formed on top of the base layer and a top layer comprising a thin monocrystal.
- Power Silicon-On-Insulator substrates address the requirements for integrating, for example, high-voltage and analog functions in intelligent, energy-efficient and highly reliable power IC devices, for automotive and industry markets. They provide excellent electrical isolation and are perfect for integrating devices operating at different voltages from a few volts to several hundred volts while reducing die area and improving reliability. These substrates are ideal for applications such as CAN/LIN transceivers, switch mode power supplies, brushless motor drivers, LED drivers, and more.
- a power SOI comprises a base layer comprising silicon, a buried insulator formed on top comprising oxide, and a top layer comprising silicon. A thickness of the buried insulator is typically between 0.4 ⁇ m to 1 ⁇ m and a thickness of the top layer is typically between 0.1 ⁇ m and 1.5 ⁇ m.
- Photonics Silicon-On-Insulator substrates address the requirement of optical function integration onto, for example, a CMOS chip for low-cost and high-speed optical transceivers.
- a substrates comprises a base layer comprising silicon, a buried insulator formed on top of the base layer and comprising oxide, and a top layer formed on top of the buried insulator and comprising monocrystalline silicon.
- a thickness of the buried insulator is typically between 0.7 ⁇ m to 2 ⁇ m and a thickness of the top layer is comprised typically between 0.1 ⁇ m and 0.5 ⁇ m.
- the crystalline silicon layer on insulator can be used to fabricate, for example, optical waveguides and other optical devices, either passive or active, e.g., through suitable implantations.
- the buried insulator enables, for example, the propagation of infrared light in the silicon layer on the basis of total internal reflection.
- the top surface of the waveguides can be either left uncovered and exposed to air, e.g., for sensing applications, or covered with a cladding, for example, made of silica.
- SOI substrates are compatible with most conventional fabrication processes.
- an SOI-based process may be implemented without special equipment or significant retooling of an existing factory.
- challenges unique to SOI are novel metrology requirements to account for the buried insulator and concerns about differential stress in the top layer comprising silicon.
- an n-type doping concentration of the top layer is within the range of 1.10 15 cm ⁇ 3 to 5.10 15 cm ⁇ 3 .
- the n-type doping of the top layer of the Silicon-On-Insulator substrate compensates and balances out for the concentration of Group III elements that diffuses from the epitaxial layers into the top layer of the Silicon-On-Insulator substrate.
- a thickness of the top layer is between 50 and 200 nm. Alternatively, a thickness of the top layer is lower than 100 nm.
- the intermediate layer confines the diffusion or migration of Group III elements within the thin silicon layer formed by the top layer.
- the intermediate layer confines the diffusion or migration of Group III elements to the surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure.
- the semiconductor structure then demonstrates improved performance at high-power and high-frequency, improved resistivity, and reduced power losses and linearity problems.
- the top layer comprises n-type doped silicon, wherein an orientation of the n-type doped silicon of the top layer is ( 111 ).
- the top layer comprises monocrystalline silicon.
- the monocrystalline silicon of the top layer can be used to fabricate, for example, optical waveguides and other optical devices, either passive or active, e.g., through suitable implantations.
- the buried insulator enables, for example, the propagation of infrared light in the silicon of the top layer on the basis of total internal reflection.
- the top surface of the waveguides manufactured within the top layer can be either left uncovered and exposed to air, e.g., for sensing applications, or covered with a cladding, for example, made of silica.
- the buried insulator comprises amorphous silicon carbide and the trap-rich layer comprises amorphous silicon carbide.
- amorphous silicon carbide acts as a trap-rich and as a barrier containing the diffusion or migration of Group III elements from the epitaxial layers of the Group III-nitride heterostructure into the Silicon-On-Insulator substrate in a surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure, for example, in the top layer and optionally close to the interface between the intermediate layer and the top layer.
- the trap-rich layer comprises silicon or polysilicon.
- the buried insulator comprises silicon dioxide and the trap-rich layer comprises silicon.
- the buried insulator comprises silicon dioxide and the trap-rich layer comprises amorphous silicon carbide.
- the trap-rich layer comprises polysilicon.
- the buried insulator comprises a layer comprising silicon nitride confined between two layers comprising silicon oxide; and the trap-rich layer comprises amorphous silicon carbide.
- the buried insulator comprises an ONO dielectric stack, wherein ONO stands for oxide-nitride-oxide.
- ONO stands for oxide-nitride-oxide.
- the buried insulator results in better thermal conduction than silicon dioxide without excessively deteriorating parasitic capacitive coupling nor jeopardizing high-speed performance of, for example, active devices manufactured from the semiconductor structure according to the present disclosure.
- the buried insulator comprising a layer comprising silicon nitride further enhances the technical effect of containing the diffusion or migration of Group III elements from the epitaxial layers of the Group III-nitride heterostructure into the Silicon-On-Insulator substrate in a surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure, for example, in the top layer and optionally close to the interface between the intermediate layer and the top layer.
- Blocking the diffusion of Group III elements from the epitaxial layers of the Group III-nitride heterostructure into the Silicon-On-Insulator substrate is more efficient in a semiconductor structure comprising a buried insulator comprising silicon nitride than in a semiconductor structure comprising a buried insulator comprising only silicon dioxide.
- the trap-rich layer comprises silicon or polysilicon.
- the silicon carbide is amorphous.
- the traps of the amorphous silicon carbide of the trap-rich layer capture the free carriers at the interface between the silicon of the top layer and the intermediate layer, thereby enabling the Silicon-On-Insulator substrate to recover its nominal resistivity, linearity, eliminating the DC dependency and leading to a substantial reduction of RF losses and crosstalk.
- a thickness of the trap-rich layer is between tens of nanometers and several micrometers.
- a thickness of the trap-rich layer comprising amorphous silicon carbide can reach a few tens of nanometers.
- a thickness of the trap-rich layer comprising polysilicon can reach a few micrometers.
- a thickness of the buried insulator is between 100 nm and 500 nm.
- a thickness of the intermediate layer comprising the buried insulator and the trap-rich layer is between a few hundreds of nanometers and a few micrometers.
- the epitaxial III-N semiconductor layer stack further comprises a spacer layer formed between the first active III-N layer and the second active III-N layer.
- the spacer layer epitaxially grown between the first active III-N layer and the second active III-N layer enhances the electron mobility within the epitaxial III-N semiconductor layer stack.
- the first active III-N layer comprises gallium nitride and wherein the second active III-N layer comprises aluminum gallium nitride.
- the first active III-N layer is grown epitaxially and comprises pure gallium nitride, preferably a monolayer of gallium nitride.
- the first active III-N layer comprises InAlGaN
- the second active III-V layer comprises InAlGaN
- the second active III-N layer comprises a bandgap larger than a bandgap of the first active III-N layer and the second active III-N layer comprises a polarization larger than the polarization of the first active III-N layer.
- first active III-N layer and second III-V layer causes polarization that contributes to a conductive 2DEG region near the junction between the first active III-N layer and the second active III-N layer, in particular, in the first active III-N layer that comprises a bandgap narrower than the bandgap of the second active III-N layer.
- the first active III-N layer for example, has a thickness between 20 and 500 nm, preferably between 30 and 300 nm, more preferably between 50 and 250 nm, such as, for example, from 100 to 150 nm.
- the second active III-N layer for example, has a thickness between 10to 100 nm, preferably between 20 to 50 nm. Such a combination of thicknesses provides good characteristics for the active layer, for example, in terms of the 2DEG obtained.
- the spacer layer comprises aluminum nitride.
- the spacer layer is grown epitaxially and comprises pure aluminum nitride.
- a thickness of the spacer layer is lower than 2 nm.
- the spacer layer is kept thin enough to minimize the roughness of the spacer layer. With minimized roughness, the spacer layer prevents the diffusion or the migration of Group III atoms into at least the first active III-N layer. This way, the thermal stability of the semiconductor structure is further improved. In other words, the thinner the spacer layer, the better the thermal stability of the semiconductor structure.
- the thickness of the spacer layer is between 0.5 nm and 1.5 nm. Even more preferably, the thickness of the spacer layer is between 0.8 nm and 1 nm.
- the epitaxial III-N semiconductor layer stack further comprises an epitaxially grown buffer layer grown between the substrate and the epitaxial active layer.
- the buffer layer may be of a different nature than the substrate, in that, for instance, the bandgap of the substrate and buffer layer are relatively far apart such as 1.1 eV and 6.2 eV, respectively, in the sense that the buffer layer has a high bandgap, in order to provide present characteristics, such as high break down voltage, e.g., higher than 250 V, preferably higher than 500 V, even more preferably higher than 1000 V, such as higher than 2000 V, or even much higher.
- the buffer layer is, for example, a III-V buffer layer with a high bandgap.
- III refers to Group III elements, such as B, Al, Ga, In, TI, Sc, Y and Lanthanide and Actinide series.
- V refers to Group V elements, such as N, P, As, Sb, Bi.
- the buffer layer may comprise a stack of layers, in an example typically the first one being a nucleation layer.
- the semiconductor structure further comprises a passivation stack formed on top of the epitaxial III-N semiconductor layer.
- the passivation stack is formed in-situ with the formation of the epitaxial III-N semiconductor layer stack.
- the passivation stack is, for example, formed on top of the second active III-N layer. This way, a fully crystalline passivation stack is epitaxially grown on top of the epitaxial III-N semiconductor layer stack. Alternatively, a partially crystalline passivation stack is epitaxially grown on top of the epitaxial III-N semiconductor layer stack.
- the passivation stack may also be formed by ex-situ deposition with the help of epitaxy tools like atomic layer deposition, also referred to as ALD, chemical vapor deposition, also referred to as CVD, or physical vapor deposition, also referred to as PVD.
- the passivation stack may be formed by in-situ deposition in a MOCVD or an MBE chamber.
- the passivation stack may be formed by depositing an amorphous film of the same material and recrystallizing it using thermal anneal.
- the passivation stack on top of the second active III-N layer for example, comprises Gallium Nitride.
- the passivation stack on top of the second active III-N layer comprises Gallium Nitride and Silicon Nitride.
- a passivation stack is formed between the epitaxial III-N semiconductor layer stack and, for example, a gate of a transistor.
- the passivation stack may be formed only under the gate and may serve additionally as gate dielectric.
- the passivation stack may be formed on top of the epitaxial III-N semiconductor layer stack and may fully cover the epitaxial III-N semiconductor layer stack.
- the passivation stack may be formed on top of the epitaxial III-N semiconductor layer stack and partially cover the surface of the epitaxial III-N semiconductor layer stack, for example, it may be formed in the ungated area between the source and the drain of a high mobility electron transistor, where it serves as passivation and prevents the depletion of the underlying 2DEG.
- the passivation stack further comprises an oxide layer and/or silicon nitride.
- the passivation layer of the semiconductor structure comprises silicon nitride and/or an oxide layer that acts as a passivation layer.
- the oxide layer exhibits an electrically clean interface to the second active III-N layer, a high dielectric constant to maximize electrostatic coupling between electrical contacts formed onto the semiconductor structure and the 2DEG, which results in an increase of, for example, the transconductance of high electron mobility transistors manufactured with the semiconductor structure and a sufficient thickness to avoid dielectric breakdown and leakage by quantum tunneling.
- a method for manufacturing a semiconductor structure comprising the steps of:
- presence of p-type dopants at the interface between the Group III-nitride heterostructure and a silicon substrate onto which the Group III-nitride heterostructure is, for example, epitaxially grown can be measured with, for example, spreading resistance profiling measurements.
- Such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of impurities from the initial growth layer of the epitaxial layers of the Group III-nitride heterostructure to the silicon substrate.
- the impurities act as a p-type impurity for the silicon substrate. More particularly, such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of Group III elements into the silicon substrate in which they act as p-type impurities for the silicon substrate.
- the diffusion or migration of Group III elements from the epitaxial layers of the Group III-nitride heterostructure into the Silicon-On-Insulator substrate is contained in a surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure, for example, in the top layer and optionally close to the interface between the intermediate layer and the top layer.
- the intermediate layer of the Silicon-On-Insulator substrate confines the diffusion or migration of Group III elements within the surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure, for example, in the top layer and optionally close to the interface between the intermediate layer and the top layer, thereby shortening the diffusion distance of the impurities into the Silicon-On-Insulator substrate.
- the n-type doping of the top layer of the Silicon-On-Insulator substrate compensates for the concentration of Group III elements that diffuses from the epitaxial layers into the Silicon-On-Insulator substrate.
- the n-type doping of the top layer of the Silicon-On-Insulator substrate balances out a concentration of p-type dopants at the interface between the epitaxial layers and the Silicon-On-Insulator substrate, wherein the concentration of these p-type dopants results from a diffusion of Group III atoms from the epitaxial III-N semiconductor layer stack into the top layer of the Silicon-On-Insulator substrate.
- the semiconductor structure manufactured with the method according to the present disclosure demonstrates improved performance at high-power and high-frequency, improved resistivity, and reduced power losses and linearity problems.
- the epitaxial III-N semiconductor layer stack comprises an epitaxial active layer that comprises the first active III-N layer, optionally a spacer layer, and the second active III-N layer.
- the epitaxial active layer is formed in-situ by epitaxial growth in a metal-organic chemical vapor deposition epitaxial chamber, also referred to as MOCVD, or in a metal-organic vapor phase epitaxial chamber, also referred to as MOVPE, or in a molecular beam epitaxial chamber, also referred to as MBE, or in a chemical beam epitaxial chamber, also referred to as CBE.
- the semiconductor structure can be formed by epitaxial growth by metal-organic chemical vapor deposition (MOCVD) or metal-organic vapor phase epitaxy (MOVPE) or be molecular beam epitaxy (MBE) or chemical beam epitaxy (CBE).
- MOCVD metal-organic chemical vapor deposition
- MOVPE metal-organic vapor phase epitaxy
- MBE molecular beam epitaxy
- CBE chemical beam epitaxy
- the epitaxial III-N semiconductor layer stack is epitaxially grown on a Silicon-On-Insulator substrate, typically at pressures, for example, between 5 mBar and 1 Bar and typically at temperatures, for example, between 600° C. and 1200° C.
- the precursor materials can be but are not limited to ammonia (NH 3 ) for nitrogen; tri-methyl-Ga (TMGa) or tri-ethyl-Ga (TEGa) for gallium, tri-methyl-Al (TMAl) or tri-ethyl-Al (TEAl) for aluminum; tri-methyl-Indium (TMIn) for indium; and silane (SiH 4 ) or disilane (SiH 3 ) 2 for silicon.
- NH 3 ammonia
- TMGa tri-methyl-Ga
- TMGa tri-ethyl-Ga
- TMGa tri-ethyl-Ga
- TMAl tri-ethyl-Al
- TMIn tri-methyl-Indium
- SiH 4 silane
- SiH 3 disilane
- the Silicon-On-Insulator substrate may comprise a buried insulator that comprises silicon oxide.
- the Silicon-On-Insulator substrate may then be produced by several methods such as, for example, a Separation by IMplantation of Oxygen, known as SIMOX, or wafer bonding, or by a seed method.
- the providing a top layer comprising n-type doped silicon comprises doping the silicon of the top layer by thermal diffusion of n-type dopants into the silicon of the top layer.
- an n-type doping concentration of the top layer is within the range of 1.10 15 cm ⁇ 3 to 5.10 15 cm ⁇ 3 .
- the providing a top layer comprising n-type doped silicon comprises doping the silicon of the top layer by ion implantation of n-type dopants into the silicon of the top layer.
- an n-type doping concentration of the top layer is within the range of 1.10 15 cm ⁇ 3 to 5.10 15 cm ⁇ 3 .
- the n-type dopants comprise one or more of the following:
- FIGS. 1 A and 1 B schematically depict an example embodiment according to the prior art of measurements performed with spreading resistance profiling on gallium-nitride epitaxially grown onto a silicon substrate.
- FIG. 2 schematically depicts an example embodiment of a semiconductor structure according to the present disclosure.
- FIG. 3 schematically depicts an example embodiment of a semiconductor structure according to the present disclosure, wherein the buried insulator comprises a layer comprising silicon nitride confined between two layers comprising silicon dioxide.
- FIG. 4 schematically depicts an example embodiment of a semiconductor structure according to the present disclosure, wherein the epitaxial III-N semiconductor layer stack further comprises a spacer between the first active III-N layer and the second active III-N layer.
- FIG. 1 A schematically illustrates an example embodiment according to the prior art of measurements performed with spreading resistance profiling on gallium-nitride epitaxially grown onto a silicon substrate.
- FIG. 1 A schematically illustrates the resistivity 91 in logarithmic scale of a sample comprising gallium-nitride epitaxially grown on silicon as a function of depth 92 within the gallium-nitride on silicon heterostructure.
- the section 93 corresponds to gallium nitride and the section 95 corresponds to a portion of the silicon substrate.
- the section 94 on FIG. 1 A corresponds to the interface between the gallium nitride and the silicon substrate. As visible on FIG.
- the resistivity 96 measured within the gallium nitride is almost constant throughout the layer and equal to 1.10 6 Ohm ⁇ cm, while the resistivity 98 measured from almost 1 ⁇ m within the silicon substrate is almost constant and equal to 1.10 4 Ohm ⁇ cm.
- a significant drop in resistivity 97 is measured by spreading resistance profiling. More precisely, the resistivity 97 in section 94 of the heterostructure drops from 1.10 6 Ohm ⁇ cm to 1.10 1 Ohm ⁇ cm before slowly increasing back to 1.10 4 Ohm ⁇ cm deeper into the silicon substrate. As visible on FIG. 1 A , the drop in resistivity 97 extends over 0.5 ⁇ m to almost 1 ⁇ m into the silicon substrate.
- FIG. 1 B schematically illustrates a concentration of species in logarithmic scale and their type within the same sample comprising gallium-nitride epitaxially grown on a silicon substrate as characterized on FIG. 1 A .
- the section 93 corresponds to gallium nitride and the section 95 corresponds to a portion of the silicon substrate.
- the section 94 on FIG. 1 B corresponds to the interface between the gallium nitride and the silicon substrate.
- gallium-nitride in this sample is almost undoped and demonstrating a concentration 81 lower than 2.10 10 atoms ⁇ cm ⁇ 3
- the silicon substrate is this sample demonstrates from almost 1 ⁇ m within the silicon substrate a concentration 83 varying from 2.10 11 atoms ⁇ cm ⁇ 3 to 6.10 11 atoms ⁇ cm ⁇ 3
- a significant concentration 82 of p-type dopants is measured by spreading resistance profiling.
- this concentration 82 increases from 2.10 10 atoms ⁇ cm ⁇ 3 close to the gallium nitride to reach 2.10 15 atoms ⁇ cm ⁇ 3 in section 94 and the concentration 82 then slowly decreases again into the silicon substrate to a concentration of 2.10 11 atoms ⁇ cm ⁇ 3 .
- Conclusion can be drawn from such spreading resistance profiling measurements that a high concentration of p-type dopants is present at the interface between gallium nitride and silicon and extending over 0.5 ⁇ m to almost 1 ⁇ m into the silicon substrate.
- FIG. 2 schematically depicts a cross-section of an example embodiment of a semiconductor structure 1 according to the present disclosure, wherein the cross-section is performed along a plane comprising a growth direction 2 , and a traverse direction 3 traverse to the growth direction 2 .
- a third direction 4 is traverse to the growth direction 2 and to the traverse direction 3 .
- the semiconductor structure 1 comprises a Silicon-On-Insulator substrate 101 and an epitaxial III-N semiconductor layer stack 202 on top of the Silicon-On-Insulator substrate 101 .
- the Silicon-On-Insulator substrate 101 comprises a base layer 10 , an intermediate layer 11 formed on top of the base layer 10 , and a top layer 12 formed on top of the intermediate layer 11 .
- the base layer 10 comprises silicon.
- the resistivity of the base layer 10 is typically between 3 and 5kOhm ⁇ cm, higher than 1 kOhm ⁇ cm.
- the epitaxial III-N semiconductor layer stack 202 comprises an epitaxial active layer 20 .
- the epitaxial active layer 20 comprises a first active III-N layer 21 formed on top of the top layer 12 and a second active III-N layer formed on top of the first active III-N layer 21 .
- the first active III-N layer 21 comprises, for example, gallium nitride and the second active III-N layer 22 , for example, comprises aluminum gallium nitride.
- a two-dimensional Electron Gas 200 is formed between the first active III-N layer 21 and the second active III-N layer 22 .
- the top layer 12 comprises n-type doped silicon.
- An orientation of the silicon of the top layer 12 is ( 111 ).
- the n-type doping concentration of the top layer 12 is within the range of 1.10 15 cm ⁇ 3 to 5.10 15 cm ⁇ 3 .
- a thickness of the top layer 12 is between 50 and 200 nm. According to an alternative embodiment, a thickness of the top layer 12 is lower than 100 nm.
- the intermediate layer 11 comprises a trap-rich layer 111 and a buried insulator 121 formed on top of the trap-rich layer 111 .
- the buried insulator 121 comprises silicon dioxide and the trap-rich layer 111 comprises silicon.
- a thickness of the buried insulator 121 is between 100nm and 500nm.
- a thickness of the trap-rich layer 111 can be, for example, several micrometers.
- the buried insulator 121 comprises silicon dioxide and the trap-rich layer 111 comprises silicon carbide, for example, amorphous silicon carbide.
- a thickness of the trap-rich layer 111 can be, for example, tens of nanometers.
- FIG. 3 schematically depicts a cross-section of an example embodiment of a semiconductor structure 1 according to the present disclosure, wherein the cross-section is performed along a plane comprising a growth direction 2 , and a traverse direction 3 traverse to the growth direction 2 .
- a third direction 4 is traverse to the growth direction 2 and to the traverse direction 3 .
- Components having identical reference numbers than on FIG. 2 fulfill the same function.
- the semiconductor structure 1 comprises a Silicon-On-Insulator substrate 101 and an epitaxial III-N semiconductor layer stack 202 on top of the Silicon-On-Insulator substrate 101 .
- the Silicon-On-Insulator substrate 101 comprises a base layer 10 , an intermediate layer 11 formed on top of the base layer 10 , and a top layer 12 formed on top of the intermediate layer 11 .
- the base layer 10 comprises silicon.
- the resistivity of the base layer 10 is typically between 3 and 5kOhm ⁇ cm, higher than 1 kOhm ⁇ cm.
- the epitaxial III-N semiconductor layer stack 202 comprises an epitaxial active layer 20 .
- the epitaxial active layer 20 comprises a first active III-N layer 21 formed on top of the top layer 12 and a second active III-N layer formed on top of the first active III-N layer 21 .
- the first active III-N layer 21 comprises, for example, gallium nitride and the second active III-N layer 22 , for example, comprises aluminum gallium nitride.
- a two-dimensional Electron Gas 200 is formed between the first active III-N layer 21 and the second active III-N layer 22 .
- the top layer 12 comprises n-type doped silicon. An orientation of the silicon of the top layer 12 is ( 111 ).
- the n-type doping concentration of the top layer 12 is within the range of 1.10 15 cm ⁇ 3 to 5.10 15 cm ⁇ 3 .
- a thickness of the top layer 12 is between 50 and 200 nm. According to an alternative embodiment, a thickness of the top layer 12 is lower than 100nm.
- the intermediate layer 11 comprises a trap-rich layer 111 and a buried insulator 121 formed on top of the trap-rich layer 111 .
- the buried insulator 121 comprises a layer 131 comprising silicon nitride confined between two layers 132 ; 133 comprising silicon oxide and the trap-rich layer 111 comprises silicon carbide, for example, amorphous silicon carbide.
- the buried insulator 121 comprises silicon dioxide and the trap-rich layer 111 comprises silicon carbide, for example, amorphous silicon carbide.
- a thickness of the buried insulator 121 is between 100 nm and 500 nm.
- a thickness of the trap-rich layer 111 can be, for example, tens of nanometers.
- the buried insulator 121 comprises silicon dioxide and the trap-rich layer 111 comprises silicon.
- a thickness of the trap-rich layer 111 can be, for example, several micrometers.
- FIG. 4 schematically depicts a cross-section of an example embodiment of a semiconductor structure 1 according to the present disclosure, wherein the cross-section is performed along a plane comprising a growth direction 2 , and a traverse direction 3 traverse to the growth direction 2 .
- a third direction 4 is traverse to the growth direction 2 and to the traverse direction 3 .
- Components having identical reference numbers in FIG. 2 or FIG. 3 fulfill the same function.
- the semiconductor structure 1 comprises a Silicon-On-Insulator substrate 101 and an epitaxial III-N semiconductor layer stack 202 on top of the Silicon-On-Insulator substrate 101 .
- the Silicon-On-Insulator substrate 101 comprises a base layer 10 , an intermediate layer 11 formed on top of the base layer 10 , and a top layer 12 formed on top of the intermediate layer 11 .
- the base layer 10 comprises silicon.
- the resistivity of the base layer 10 is typically between 3 and 5 kOhm ⁇ cm, higher than 1 kOhm ⁇ cm.
- the epitaxial III-N semiconductor layer stack 202 comprises an epitaxial active layer 20 .
- the epitaxial active layer 20 comprises a first active III-N layer 21 formed on top of the top layer 12 , a spacer layer 23 formed on top of the first active III-N layer 21 , and a second active III-N layer formed on top of the spacer layer 23 .
- the first active III-N layer 21 comprises, for example, gallium nitride and the second active III-N layer 22 , for example, comprises aluminum gallium nitride.
- the spacer layer 23 preferably comprises aluminum nitride.
- a two-dimensional Electron Gas 200 is formed between the first active III-N layer 21 and the second active III-N layer 22 .
- the top layer 12 comprises n-type doped silicon. An orientation of the silicon of the top layer 12 is ( 111 ).
- the n-type doping concentration of the top layer 12 is within the range of 1.10 15 cm ⁇ 3 to 5.10 15 cm ⁇ 3 .
- a thickness of the top layer 12 is between 50 and 200 nm. According to an alternative embodiment, a thickness of the top layer 12 is lower than 100 nm.
- the intermediate layer 11 comprises a trap-rich layer 111 and a buried insulator 121 formed on top of the trap-rich layer 111 .
- the buried insulator 121 comprises silicon dioxide and the trap-rich layer 111 comprises silicon.
- a thickness of the buried insulator 121 is between 100 nm and 500 nm.
- a thickness of the trap-rich layer 111 can be, for example, several micrometers.
- the buried insulator 121 comprises silicon dioxide and the trap-rich layer 111 comprises silicon carbide, for example, amorphous silicon carbide.
- a thickness of the trap-rich layer 111 can be, for example, several micrometers.
Landscapes
- Engineering & Computer Science (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Condensed Matter Physics & Semiconductors (AREA)
- General Physics & Mathematics (AREA)
- Manufacturing & Machinery (AREA)
- Computer Hardware Design (AREA)
- Physics & Mathematics (AREA)
- Power Engineering (AREA)
- Chemical & Material Sciences (AREA)
- Materials Engineering (AREA)
- Crystallography & Structural Chemistry (AREA)
- Recrystallisation Techniques (AREA)
- Junction Field-Effect Transistors (AREA)
Abstract
Description
- This application is a national phase entry under 35 U.S.C. § 371 of International Patent Application PCT/EP2022/082085, filed Nov. 16, 2022, designating the United States of America and published as International Patent Publication WO 2023/110267 Al on Jun. 22, 2023, which claims the benefit under Article 8 of the Patent Cooperation Treaty to French Patent Application Serial No. FR2113655, filed Dec. 16, 2021.
- The present disclosure generally relates, amongst others, to a semiconductor structure and to a method of growing thereof. More particularly, it relates to a semiconductor structure comprising Group III-nitride grown onto Silicon-On-Insulator, wherein the semiconductor structure achieves outstanding performance for high-power and high-frequency applications, and to a method of growing thereof.
- Group III-nitride-based heterostructures are very suited for high-power and high-frequency applications due to their high electron velocity and high critical electric field. For example, AlGaN/GaN heterostructures are conventionally used for the manufacturing of field effect transistors also called FETs. In this heterostructure, a two dimensional electron gas, also referred to as 2DEG, is generated by the spontaneous and piezoelectric polarization between the two active layers, i.e., between AlGaN and GaN.
- Group III-nitride-based heterostructures are typically manufactured on top of conventional silicon substrates. With the ever increasing need for high-power and high-frequency solutions, the telecommunication industry is faced with the challenge of making such Group III-nitride-based heterostructures compatible with existing technologies. For example, Group III-nitride-based heterostructures should allow the continued miniaturization of microelectronic devices and the continued improvement of their performance.
- For high-power and high-frequency applications, it is essential to maximize the resistivity of the underlying substrate of the devices. However, measurements performed with spreading resistance profiling on gallium-nitride epitaxially grown onto a silicon substrate demonstrate a significant drop in resistivity versus depth in the heterostructure.
- More generally, measurements performed with spreading resistance profiling on Group III-nitride heterostructures epitaxially grown on a silicon substrate demonstrate a similar drop in resistivity at the interface between the Group III-nitride heterostructure and the silicon substrate and similar presence of p-type dopants at the interface between the Group III-nitride heterostructure and the silicon substrate. Such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of impurities from the initial growth layer of the epitaxial layers of the Group III-nitride heterostructure to the silicon substrate. The impurities act as a p-type impurity for the silicon substrate. More particularly, such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of Group III elements into the silicon substrate in which they act as p-type impurities for the silicon substrate. For example, in the sample investigated in
FIGS. 1A and 1B of the present disclosure, such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of gallium and/or aluminum into the silicon substrate. Gallium and/or aluminum act as p-type impurities for silicon and thereby change the resistivity of the silicon substrate. - Several problems arise from such diffusion of Group III elements into the silicon substrate. For high-power and high-frequency applications, the presence of a high concentration of p-type dopants at the interface between gallium nitride and silicon will cause a capacitive coupling resulting in significant power dissipation and RF losses for components manufactured from this structure. Additionally, the diffusion of Group III elements into the silicon substrate will cause linearity problems to arise due to the generation of harmonic frequencies in components manufactured from this structure.
- It is thus an object of embodiments of the present disclosure to propose a semiconductor structure and a manufacturing method that do not show the inherent shortcomings of the prior art. More specifically, it is an object of embodiments of the present disclosure to propose a semiconductor structure with improved performance at high-power and high-frequency and a manufacturing method thereof.
- There is a need for a semiconductor structure that demonstrates improved resistivity, and reduced power losses and linearity problems. Additionally, there is a need for a semiconductor structure that, from a manufacturing perspective, is compatible with existing technologies.
- This object is achieved, according to a first example aspect of the present disclosure, by a semiconductor structure comprising:
-
-
- a Silicon-On-Insulator substrate comprising:
- a base layer comprising silicon;
- an intermediate layer formed on top of the base layer; and
- a top layer formed on top of the intermediate layer;
- an epitaxial III-N semiconductor layer stack on top of the Silicon-On-Insulator substrate, the epitaxial III-N semiconductor layer stack comprising an epitaxial active layer; wherein the epitaxial active layer comprises:
- a first active III-N layer formed on top of the top layer;
- a second active III-N layer formed on top of the first active III-N layer;
- with a two dimensional Electron Gas between the first active III-N layer and the second active III-N layer;
- a Silicon-On-Insulator substrate comprising:
- and wherein:
- the top layer comprises n-type doped silicon; and
- the intermediate layer comprises:
- a trap-rich layer; and
- a buried insulator formed on top of a trap-rich layer.
-
- As previously mentioned, presence of p-type dopants at the interface between the Group III-nitride heterostructure and a silicon substrate onto which the Group III-nitride heterostructure is, for example, epitaxially grown can be measured with, for example, spreading resistance profiling measurements. Such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of impurities from the initial growth layer of the epitaxial layers of the Group III-nitride heterostructure to the silicon substrate. The impurities act as a p-type impurity for the silicon substrate. More particularly, such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of Group III elements into the silicon substrate in which they act as p-type impurities for the silicon substrate.
- With the semiconductor structure according to the present disclosure, the diffusion or migration of Group III elements from the epitaxial layers of the Group III-nitride heterostructure into the Silicon-On-Insulator substrate is contained in a surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure, for example, in the top layer and optionally close to the interface between the intermediate layer and the top layer. Indeed, the intermediate layer of the Silicon-On-Insulator substrate according to the present disclosure confines the diffusion or migration of Group III elements within the surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure, for example, in the top layer and optionally close to the interface between the intermediate layer and the top layer, thereby shortening the diffusion distance of the impurities into the Silicon-On-Insulator substrate.
- With the semiconductor structure according to the present disclosure, the n-type doping of the top layer of the Silicon-On-Insulator substrate compensates for the concentration of Group III elements that diffuses from the epitaxial layers into the Silicon-On-Insulator substrate. In other words, the n-type doping of the top layer of the Silicon-On-Insulator substrate according to the present disclosure balances out a concentration of p-type dopants at the interface between the epitaxial layers and the Silicon-On-Insulator substrate, wherein the concentration of these p-type dopants results from a diffusion of Group III atoms from the epitaxial III-N semiconductor layer stack into the top layer of the Silicon-On-Insulator substrate.
- This way, the semiconductor structure according to the present disclosure demonstrates improved performance at high-power and high-frequency, improved resistivity, and reduced power losses and linearity problems.
- The use of a trap-rich layer has been proven as one of the most effective techniques to reduce these parasitic effects and to enhance the high-resistivity properties of silicon, while being compatible with industrial SOI wafer fabrication and with the important thermal budget of standard CMOS process. The traps of the trap-rich layer capture the free carriers at the interface between the silicon and the intermediate layer, thereby enabling the Silicon-On-Insulator substrate to recover its nominal resistivity, linearity, eliminating the DC dependency and leading to a substantial reduction of RF losses and crosstalk. In the context of the present disclosure, the trap-rich layer has a defect density suitable for trapping free charges that may be generated in the Silicon-On-Insulator substrate. The trap-rich layer may provide a trapping effect as well. The trap-rich layer has a thickness of several tens of nanometers to several microns, for example, 50 nm to 3 microns. The trap-rich layer comprises silicon, or amorphous silicon carbide, or polycrystalline silicon also referred to as polysilicon.
- In the context of the present disclosure, a two-dimensional electron gas, also referred to as 2DEG, is a gas of electrons free to move in two dimensions, but tightly confined in the first. This tight confinement leads to quantized energy levels for motion in that direction. The electrons appear to be a 2D sheet embedded in a 3D world.
- In the context of the present disclosure, Group III-nitride refers to semiconductor compounds formed between elements in Group III of the periodic table, for example, Boron, also referred to as B, Aluminum, also referred to as Al, Gallium, also referred to as Ga, Indium, also referred to as In, and Nitrogen, also referred to as N. Example of binary Group III-nitride compounds are GaN, AIN, BN, etc. Group III-nitride also refers to ternary and quaternary compounds such as, for example, AlGaN and InAlGaN.
- In the context of the present disclosure, the first active III-N layer comprises one or more of N, P, As, and one or more of B, Al, Ga, In and Tl. The first active III-N layer, for example, comprises GaN. The second active III-N layer comprises one or more of N, P, As, and one or more of B, Al, Ga, In, and Tl. The second active III-N layer, for example, comprises AlGaN. The term AlGaN relates to a composition comprising Al, Ga and N in any stoichiometric ratio (AlxGayN) wherein x is between 0 and 1 and y is between 0 and 1. Alternatively, the second active III-N layer, for example, comprises AIN. Alternatively, the second active III-N layer comprises InAlGaN. A composition such as InAlGaN comprises In in any suitable amount. Alternatively, both first active III-N layer and second active III-N layer comprise InAlGaN, and the second active III-N layer comprises a bandgap larger than a bandgap of the first active III-N layer and wherein the second active III-N layer comprises a polarization larger than the polarization of the first active III-N layer. Alternatively, both first active III-N layer and second active III-N layer comprise BInAlGaN, and the second active III-N layer comprises a bandgap larger than a bandgap of the first active III-N layer and wherein the second active III-N layer comprises a polarization larger than the polarization of the first active III-N layer. Compositions of the active layer may be chosen in view of characteristics to be obtained, and compositions may vary accordingly. For example, good results were obtained with a first active III-N layer comprising GaN of about 150 nm thickness and a second active III-N layer comprising AlGaN of about 20 nm thickness.
- In the context of the present disclosure, the base layer of the Silicon-On-Insulator substrate comprises bulk silicon and a resistivity of the base layer of the Silicon-On-Insulator substrate is typically between 3 and 5 kOhm·cm, and is preferably higher than 1 kOhm·cm. This way, the resistivity of the substrate underlying the epitaxial III-N semiconductor layer stack is maximized for high-power and high-frequency applications.
- In the context of the present disclosure, the technology of Silicon-On-Insulator, also referred to as SOI, corresponds to the manufacturing of semiconductor devices in a layered silicon-insulator-silicon substrate. The choice of insulator depends largely on the intended application of the semiconductor devices. Several types of Silicon-On-Insulator substrates may be used within the context of the present disclosure.
- Due to the isolation from the bulk silicon of the base layer of the Silicon-On-Insulator substrate, parasitic capacitance within the semiconductor devices manufactured from the Group III-nitride heterostructure is lowered, thereby improving their power consumption and their performance. The semiconductor devices manufactured on Silicon-On-Insulator also demonstrate a higher resistance to latchup and a higher performance at equivalent VDD than semiconductor devices integrated on other types of substrates. The temperature dependency of the semiconductor devices manufactured on SOI is reduced compared to semiconductor devices integrated on other types of substrates. Due to the isolation, the semiconductor devices manufactured on SOI demonstrate lower leakage currents and consequently higher power efficiency.
- Radio-Frequency Silicon-On-Insulator substrates, also referred to as RF-SOI substrates, enable high RF performance on silicon films compatible with standard CMOS processes, high linearity RF isolation and power signals, low RF loss, digital processing and power management integration.
- For example, an enhanced signal integrity substrate for RF application comprises a base layer comprising high-resistive silicon, a trap rich layer formed on top of the base layer, a buried insulator formed on top of the trap rich layer, and a top layer formed on top of the buried insulator, wherein the top layer comprises a monocrystal. A resistivity of the base layer is typically over 3 kOhm·cm. A thickness of the top layer is typically between 50 nm and 200 nm. The addition of a trap-rich layer provides outstanding RF performances. Such substrate is particularly suited for devices with stringent linearity specifications. Applications typically target, for example, LTE-Advanced and 5G specifications and address different performance requirements. Compared to a high-resistive SOI substrate, an enhanced signal integrity substrate demonstrates better linearity, lower RF losses, lower crosstalk, improved quality factors for passives, smaller die sizes and higher thermal conductivity. Enhanced signal integrity substrates further typically demonstrate a harmonic quality factor lower than −80 dBm.
- Another example of a RF-SOI comprises a base layer comprising mid-resistive silicon, a trap-rich layer formed on top of the base layer, a buried insulator formed on top of the trap-rich layer, and a top layer comprising a thin monocrystal. Such substrate is particularly suited for, for example, cost sensitive highly integrated devices, and is particularly well suited to, for example, WI-FI®, IoT and other consumer applications specifications.
- Another example of a RF-SOI called high-resistive SOI targets, for example, devices with lower linearity specifications and 2G and 3G specifications. Such substrate comprises a base layer comprising high-resistive silicon, a buried insulator formed on top of the base layer and a top layer comprising a thin monocrystal.
- Power Silicon-On-Insulator substrates address the requirements for integrating, for example, high-voltage and analog functions in intelligent, energy-efficient and highly reliable power IC devices, for automotive and industry markets. They provide excellent electrical isolation and are perfect for integrating devices operating at different voltages from a few volts to several hundred volts while reducing die area and improving reliability. These substrates are ideal for applications such as CAN/LIN transceivers, switch mode power supplies, brushless motor drivers, LED drivers, and more. A power SOI comprises a base layer comprising silicon, a buried insulator formed on top comprising oxide, and a top layer comprising silicon. A thickness of the buried insulator is typically between 0.4 μm to 1 μm and a thickness of the top layer is typically between 0.1 μm and 1.5 μm.
- Photonics Silicon-On-Insulator substrates address the requirement of optical function integration onto, for example, a CMOS chip for low-cost and high-speed optical transceivers. Such a substrates comprises a base layer comprising silicon, a buried insulator formed on top of the base layer and comprising oxide, and a top layer formed on top of the buried insulator and comprising monocrystalline silicon. A thickness of the buried insulator is typically between 0.7 μm to 2 μm and a thickness of the top layer is comprised typically between 0.1 μm and 0.5 μm. The crystalline silicon layer on insulator can be used to fabricate, for example, optical waveguides and other optical devices, either passive or active, e.g., through suitable implantations. The buried insulator enables, for example, the propagation of infrared light in the silicon layer on the basis of total internal reflection. The top surface of the waveguides can be either left uncovered and exposed to air, e.g., for sensing applications, or covered with a cladding, for example, made of silica.
- From a manufacturing perspective, SOI substrates are compatible with most conventional fabrication processes. In general, an SOI-based process may be implemented without special equipment or significant retooling of an existing factory. Among challenges unique to SOI are novel metrology requirements to account for the buried insulator and concerns about differential stress in the top layer comprising silicon.
- According to example embodiments, an n-type doping concentration of the top layer is within the range of 1.1015 cm−3 to 5.1015 cm−3.
- This way, the n-type doping of the top layer of the Silicon-On-Insulator substrate compensates and balances out for the concentration of Group III elements that diffuses from the epitaxial layers into the top layer of the Silicon-On-Insulator substrate.
- According to example embodiments, a thickness of the top layer is between 50 and 200 nm. Alternatively, a thickness of the top layer is lower than 100 nm.
- This way, the intermediate layer confines the diffusion or migration of Group III elements within the thin silicon layer formed by the top layer. In other words, the intermediate layer confines the diffusion or migration of Group III elements to the surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure. The semiconductor structure then demonstrates improved performance at high-power and high-frequency, improved resistivity, and reduced power losses and linearity problems.
- According to example embodiments, the top layer comprises n-type doped silicon, wherein an orientation of the n-type doped silicon of the top layer is (111).
- According to example embodiments, the top layer comprises monocrystalline silicon.
- This way, the monocrystalline silicon of the top layer can be used to fabricate, for example, optical waveguides and other optical devices, either passive or active, e.g., through suitable implantations. The buried insulator enables, for example, the propagation of infrared light in the silicon of the top layer on the basis of total internal reflection. The top surface of the waveguides manufactured within the top layer can be either left uncovered and exposed to air, e.g., for sensing applications, or covered with a cladding, for example, made of silica.
- According to example embodiments, the buried insulator comprises amorphous silicon carbide and the trap-rich layer comprises amorphous silicon carbide.
- This way, amorphous silicon carbide acts as a trap-rich and as a barrier containing the diffusion or migration of Group III elements from the epitaxial layers of the Group III-nitride heterostructure into the Silicon-On-Insulator substrate in a surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure, for example, in the top layer and optionally close to the interface between the intermediate layer and the top layer. Alternatively, the trap-rich layer comprises silicon or polysilicon.
- According to example embodiments, the buried insulator comprises silicon dioxide and the trap-rich layer comprises silicon.
- According to example embodiments, the buried insulator comprises silicon dioxide and the trap-rich layer comprises amorphous silicon carbide.
- Alternatively, the trap-rich layer comprises polysilicon.
- According to example embodiments, the buried insulator comprises a layer comprising silicon nitride confined between two layers comprising silicon oxide; and the trap-rich layer comprises amorphous silicon carbide.
- In this example embodiment, the buried insulator comprises an ONO dielectric stack, wherein ONO stands for oxide-nitride-oxide. The buried insulator results in better thermal conduction than silicon dioxide without excessively deteriorating parasitic capacitive coupling nor jeopardizing high-speed performance of, for example, active devices manufactured from the semiconductor structure according to the present disclosure. Additionally, the buried insulator comprising a layer comprising silicon nitride further enhances the technical effect of containing the diffusion or migration of Group III elements from the epitaxial layers of the Group III-nitride heterostructure into the Silicon-On-Insulator substrate in a surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure, for example, in the top layer and optionally close to the interface between the intermediate layer and the top layer. Blocking the diffusion of Group III elements from the epitaxial layers of the Group III-nitride heterostructure into the Silicon-On-Insulator substrate is more efficient in a semiconductor structure comprising a buried insulator comprising silicon nitride than in a semiconductor structure comprising a buried insulator comprising only silicon dioxide. Alternatively, the trap-rich layer comprises silicon or polysilicon.
- According to example embodiments, the silicon carbide is amorphous.
- The traps of the amorphous silicon carbide of the trap-rich layer capture the free carriers at the interface between the silicon of the top layer and the intermediate layer, thereby enabling the Silicon-On-Insulator substrate to recover its nominal resistivity, linearity, eliminating the DC dependency and leading to a substantial reduction of RF losses and crosstalk.
- According to example embodiments, a thickness of the trap-rich layer is between tens of nanometers and several micrometers. For example, a thickness of the trap-rich layer comprising amorphous silicon carbide can reach a few tens of nanometers. Alternatively, a thickness of the trap-rich layer comprising polysilicon can reach a few micrometers.
- According to example embodiments, a thickness of the buried insulator is between 100 nm and 500 nm.
- According to example embodiments, a thickness of the intermediate layer comprising the buried insulator and the trap-rich layer is between a few hundreds of nanometers and a few micrometers.
- According to example embodiments, the epitaxial III-N semiconductor layer stack further comprises a spacer layer formed between the first active III-N layer and the second active III-N layer.
- This way, the spacer layer epitaxially grown between the first active III-N layer and the second active III-N layer enhances the electron mobility within the epitaxial III-N semiconductor layer stack.
- According to example embodiments, the first active III-N layer comprises gallium nitride and wherein the second active III-N layer comprises aluminum gallium nitride.
- Preferably, the first active III-N layer is grown epitaxially and comprises pure gallium nitride, preferably a monolayer of gallium nitride.
- According to example embodiments, the first active III-N layer comprises InAlGaN, and the second active III-V layer comprises InAlGaN, and the second active III-N layer comprises a bandgap larger than a bandgap of the first active III-N layer and the second active III-N layer comprises a polarization larger than the polarization of the first active III-N layer.
- This way, the use of different materials in adjacent first active III-N layer and second III-V layer causes polarization that contributes to a conductive 2DEG region near the junction between the first active III-N layer and the second active III-N layer, in particular, in the first active III-N layer that comprises a bandgap narrower than the bandgap of the second active III-N layer.
- The first active III-N layer, for example, has a thickness between 20 and 500 nm, preferably between 30 and 300 nm, more preferably between 50 and 250 nm, such as, for example, from 100 to 150 nm. The second active III-N layer, for example, has a thickness between 10to 100 nm, preferably between 20 to 50 nm. Such a combination of thicknesses provides good characteristics for the active layer, for example, in terms of the 2DEG obtained.
- According to example embodiments, the spacer layer comprises aluminum nitride.
- Preferably, the spacer layer is grown epitaxially and comprises pure aluminum nitride.
- According to example embodiments, a thickness of the spacer layer is lower than 2 nm.
- This way, the spacer layer is kept thin enough to minimize the roughness of the spacer layer. With minimized roughness, the spacer layer prevents the diffusion or the migration of Group III atoms into at least the first active III-N layer. This way, the thermal stability of the semiconductor structure is further improved. In other words, the thinner the spacer layer, the better the thermal stability of the semiconductor structure. Preferably, the thickness of the spacer layer is between 0.5 nm and 1.5 nm. Even more preferably, the thickness of the spacer layer is between 0.8 nm and 1 nm.
- According to example embodiments, the epitaxial III-N semiconductor layer stack further comprises an epitaxially grown buffer layer grown between the substrate and the epitaxial active layer.
- The buffer layer may be of a different nature than the substrate, in that, for instance, the bandgap of the substrate and buffer layer are relatively far apart such as 1.1 eV and 6.2 eV, respectively, in the sense that the buffer layer has a high bandgap, in order to provide present characteristics, such as high break down voltage, e.g., higher than 250 V, preferably higher than 500 V, even more preferably higher than 1000 V, such as higher than 2000 V, or even much higher. The buffer layer is, for example, a III-V buffer layer with a high bandgap. Therein III refers to Group III elements, such as B, Al, Ga, In, TI, Sc, Y and Lanthanide and Actinide series. Therein V refers to Group V elements, such as N, P, As, Sb, Bi. The buffer layer may comprise a stack of layers, in an example typically the first one being a nucleation layer.
- According to example embodiments, the semiconductor structure further comprises a passivation stack formed on top of the epitaxial III-N semiconductor layer.
- The passivation stack is formed in-situ with the formation of the epitaxial III-N semiconductor layer stack. The passivation stack is, for example, formed on top of the second active III-N layer. This way, a fully crystalline passivation stack is epitaxially grown on top of the epitaxial III-N semiconductor layer stack. Alternatively, a partially crystalline passivation stack is epitaxially grown on top of the epitaxial III-N semiconductor layer stack. The passivation stack may also be formed by ex-situ deposition with the help of epitaxy tools like atomic layer deposition, also referred to as ALD, chemical vapor deposition, also referred to as CVD, or physical vapor deposition, also referred to as PVD. Alternatively, the passivation stack may be formed by in-situ deposition in a MOCVD or an MBE chamber. Alternatively, the passivation stack may be formed by depositing an amorphous film of the same material and recrystallizing it using thermal anneal. The passivation stack on top of the second active III-N layer, for example, comprises Gallium Nitride. Alternatively, the passivation stack on top of the second active III-N layer comprises Gallium Nitride and Silicon Nitride.
- A passivation stack is formed between the epitaxial III-N semiconductor layer stack and, for example, a gate of a transistor. The passivation stack may be formed only under the gate and may serve additionally as gate dielectric. Alternatively, the passivation stack may be formed on top of the epitaxial III-N semiconductor layer stack and may fully cover the epitaxial III-N semiconductor layer stack. Alternatively, the passivation stack may be formed on top of the epitaxial III-N semiconductor layer stack and partially cover the surface of the epitaxial III-N semiconductor layer stack, for example, it may be formed in the ungated area between the source and the drain of a high mobility electron transistor, where it serves as passivation and prevents the depletion of the underlying 2DEG.
- According to example embodiments, the passivation stack further comprises an oxide layer and/or silicon nitride.
- This way, the passivation layer of the semiconductor structure according to a first example aspect of the present disclosure comprises silicon nitride and/or an oxide layer that acts as a passivation layer. The oxide layer exhibits an electrically clean interface to the second active III-N layer, a high dielectric constant to maximize electrostatic coupling between electrical contacts formed onto the semiconductor structure and the 2DEG, which results in an increase of, for example, the transconductance of high electron mobility transistors manufactured with the semiconductor structure and a sufficient thickness to avoid dielectric breakdown and leakage by quantum tunneling.
- According to a second example aspect of the present disclosure, there is provided a method for manufacturing a semiconductor structure, wherein the method comprises the steps of:
-
- providing a Silicon-On-Insulator substrate comprising:
- providing a base layer comprising silicon;
- providing an intermediate layer on top of the base layer by:
- providing a trap-rich layer; and
- providing a buried insulator formed on top of the trap-rich layer; and
- providing a top layer comprising n-type doped silicon and formed on top of the intermediate layer;
- providing an epitaxial III-N semiconductor layer stack on top of the Silicon-On-Insulator substrate, the epitaxial III-N semiconductor layer stack comprising an epitaxial active layer; wherein providing the epitaxial active layer comprises the steps of:
- providing a first active III-N layer on top of the top layer;
- providing a second active III-N layer on top of the first active III-N layer;
- thereby forming a two dimensional Electron Gas between the first active III-N layer and the second active III-N layer.
- providing a Silicon-On-Insulator substrate comprising:
- As previously mentioned, presence of p-type dopants at the interface between the Group III-nitride heterostructure and a silicon substrate onto which the Group III-nitride heterostructure is, for example, epitaxially grown can be measured with, for example, spreading resistance profiling measurements. Such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of impurities from the initial growth layer of the epitaxial layers of the Group III-nitride heterostructure to the silicon substrate. The impurities act as a p-type impurity for the silicon substrate. More particularly, such presence of p-type dopants at the interface between Group III-nitride heterostructure and silicon is attributed to the diffusion or migration of Group III elements into the silicon substrate in which they act as p-type impurities for the silicon substrate.
- With the method for manufacturing a semiconductor structure according to the present disclosure, the diffusion or migration of Group III elements from the epitaxial layers of the Group III-nitride heterostructure into the Silicon-On-Insulator substrate is contained in a surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure, for example, in the top layer and optionally close to the interface between the intermediate layer and the top layer. Indeed, with the method according to the present disclosure, the intermediate layer of the Silicon-On-Insulator substrate confines the diffusion or migration of Group III elements within the surface region of the Silicon-On-Insulator substrate close to the epitaxial layers of the Group III-nitride heterostructure, for example, in the top layer and optionally close to the interface between the intermediate layer and the top layer, thereby shortening the diffusion distance of the impurities into the Silicon-On-Insulator substrate.
- With the method for manufacturing a semiconductor structure according to the present disclosure, the n-type doping of the top layer of the Silicon-On-Insulator substrate compensates for the concentration of Group III elements that diffuses from the epitaxial layers into the Silicon-On-Insulator substrate. In other words, the n-type doping of the top layer of the Silicon-On-Insulator substrate balances out a concentration of p-type dopants at the interface between the epitaxial layers and the Silicon-On-Insulator substrate, wherein the concentration of these p-type dopants results from a diffusion of Group III atoms from the epitaxial III-N semiconductor layer stack into the top layer of the Silicon-On-Insulator substrate.
- This way, the semiconductor structure manufactured with the method according to the present disclosure demonstrates improved performance at high-power and high-frequency, improved resistivity, and reduced power losses and linearity problems.
- The epitaxial III-N semiconductor layer stack comprises an epitaxial active layer that comprises the first active III-N layer, optionally a spacer layer, and the second active III-N layer. The epitaxial active layer is formed in-situ by epitaxial growth in a metal-organic chemical vapor deposition epitaxial chamber, also referred to as MOCVD, or in a metal-organic vapor phase epitaxial chamber, also referred to as MOVPE, or in a molecular beam epitaxial chamber, also referred to as MBE, or in a chemical beam epitaxial chamber, also referred to as CBE.
- The semiconductor structure can be formed by epitaxial growth by metal-organic chemical vapor deposition (MOCVD) or metal-organic vapor phase epitaxy (MOVPE) or be molecular beam epitaxy (MBE) or chemical beam epitaxy (CBE). In the MOVPE or in the MOCVD process, the epitaxial III-N semiconductor layer stack is epitaxially grown on a Silicon-On-Insulator substrate, typically at pressures, for example, between 5 mBar and 1 Bar and typically at temperatures, for example, between 600° C. and 1200° C. The precursor materials can be but are not limited to ammonia (NH3) for nitrogen; tri-methyl-Ga (TMGa) or tri-ethyl-Ga (TEGa) for gallium, tri-methyl-Al (TMAl) or tri-ethyl-Al (TEAl) for aluminum; tri-methyl-Indium (TMIn) for indium; and silane (SiH4) or disilane (SiH3)2 for silicon.
- The Silicon-On-Insulator substrate may comprise a buried insulator that comprises silicon oxide. The Silicon-On-Insulator substrate may then be produced by several methods such as, for example, a Separation by IMplantation of Oxygen, known as SIMOX, or wafer bonding, or by a seed method.
- According to example embodiments, the providing a top layer comprising n-type doped silicon comprises doping the silicon of the top layer by thermal diffusion of n-type dopants into the silicon of the top layer.
- Preferably, an n-type doping concentration of the top layer is within the range of 1.1015 cm−3 to 5.1015 cm−3.
- According to example embodiments, the providing a top layer comprising n-type doped silicon comprises doping the silicon of the top layer by ion implantation of n-type dopants into the silicon of the top layer.
- Preferably, an n-type doping concentration of the top layer is within the range of 1.1015 cm−3 to 5.1015 cm−3.
- According to example embodiments, the n-type dopants comprise one or more of the following:
-
- Phosphorus;
- Arsenic;
- Antimony.
- Some example embodiments will now be described with reference to the accompanying drawings.
-
FIGS. 1A and 1B schematically depict an example embodiment according to the prior art of measurements performed with spreading resistance profiling on gallium-nitride epitaxially grown onto a silicon substrate. -
FIG. 2 schematically depicts an example embodiment of a semiconductor structure according to the present disclosure. -
FIG. 3 schematically depicts an example embodiment of a semiconductor structure according to the present disclosure, wherein the buried insulator comprises a layer comprising silicon nitride confined between two layers comprising silicon dioxide. -
FIG. 4 schematically depicts an example embodiment of a semiconductor structure according to the present disclosure, wherein the epitaxial III-N semiconductor layer stack further comprises a spacer between the first active III-N layer and the second active III-N layer. -
FIG. 1A schematically illustrates an example embodiment according to the prior art of measurements performed with spreading resistance profiling on gallium-nitride epitaxially grown onto a silicon substrate. Indeed,FIG. 1A schematically illustrates theresistivity 91 in logarithmic scale of a sample comprising gallium-nitride epitaxially grown on silicon as a function ofdepth 92 within the gallium-nitride on silicon heterostructure. OnFIG. 1A , thesection 93 corresponds to gallium nitride and thesection 95 corresponds to a portion of the silicon substrate. Thesection 94 onFIG. 1A corresponds to the interface between the gallium nitride and the silicon substrate. As visible onFIG. 1A , theresistivity 96 measured within the gallium nitride is almost constant throughout the layer and equal to 1.106 Ohm·cm, while theresistivity 98 measured from almost 1 μm within the silicon substrate is almost constant and equal to 1.104 Ohm·cm. However, at theinterface 94 between the gallium nitride and the silicon substrate, and as visible onFIG. 1A , a significant drop inresistivity 97 is measured by spreading resistance profiling. More precisely, theresistivity 97 insection 94 of the heterostructure drops from 1.106 Ohm·cm to 1.101 Ohm·cm before slowly increasing back to 1.104 Ohm·cm deeper into the silicon substrate. As visible onFIG. 1A , the drop inresistivity 97 extends over 0.5 μm to almost 1 μm into the silicon substrate. - The drop in resistivity at the interface between the gallium nitride and the silicon substrate is further investigated with spreading resistance profiling measurements. The results of such measurements are, for example, depicted on
FIG. 1B .FIG. 1B schematically illustrates a concentration of species in logarithmic scale and their type within the same sample comprising gallium-nitride epitaxially grown on a silicon substrate as characterized onFIG. 1A . OnFIG. 1B , thesection 93 corresponds to gallium nitride and thesection 95 corresponds to a portion of the silicon substrate. Thesection 94 onFIG. 1B corresponds to the interface between the gallium nitride and the silicon substrate. As visible onFIG. 1B , gallium-nitride in this sample is almost undoped and demonstrating aconcentration 81 lower than 2.1010 atoms·cm−3, while the silicon substrate is this sample demonstrates from almost 1 μm within the silicon substrate aconcentration 83 varying from 2.1011 atoms·cm−3 to 6.1011 atoms·cm−3. However, at theinterface 94 between the gallium nitride and the silicon substrate, and as visible onFIG. 1B , asignificant concentration 82 of p-type dopants is measured by spreading resistance profiling. More precisely, thisconcentration 82 increases from 2.1010 atoms·cm−3 close to the gallium nitride to reach 2.1015 atoms·cm−3 insection 94 and theconcentration 82 then slowly decreases again into the silicon substrate to a concentration of 2.1011 atoms·cm−3. Conclusion can be drawn from such spreading resistance profiling measurements that a high concentration of p-type dopants is present at the interface between gallium nitride and silicon and extending over 0.5 μm to almost 1 μm into the silicon substrate. -
FIG. 2 schematically depicts a cross-section of an example embodiment of asemiconductor structure 1 according to the present disclosure, wherein the cross-section is performed along a plane comprising agrowth direction 2, and atraverse direction 3 traverse to thegrowth direction 2. Athird direction 4 is traverse to thegrowth direction 2 and to thetraverse direction 3. Thesemiconductor structure 1 comprises a Silicon-On-Insulator substrate 101 and an epitaxial III-Nsemiconductor layer stack 202 on top of the Silicon-On-Insulator substrate 101. The Silicon-On-Insulator substrate 101 comprises abase layer 10, anintermediate layer 11 formed on top of thebase layer 10, and atop layer 12 formed on top of theintermediate layer 11. Thebase layer 10 comprises silicon. The resistivity of thebase layer 10 is typically between 3 and 5kOhm·cm, higher than 1 kOhm·cm. The epitaxial III-Nsemiconductor layer stack 202 comprises an epitaxialactive layer 20. The epitaxialactive layer 20 comprises a first active III-N layer 21 formed on top of thetop layer 12 and a second active III-N layer formed on top of the first active III-N layer 21. The first active III-N layer 21 comprises, for example, gallium nitride and the second active III-N layer 22, for example, comprises aluminum gallium nitride. A two-dimensional Electron Gas 200 is formed between the first active III-N layer 21 and the second active III-N layer 22. Thetop layer 12 comprises n-type doped silicon. An orientation of the silicon of thetop layer 12 is (111). The n-type doping concentration of thetop layer 12 is within the range of 1.1015 cm−3 to 5.1015 cm−3. A thickness of thetop layer 12 is between 50 and 200 nm. According to an alternative embodiment, a thickness of thetop layer 12 is lower than 100 nm. Theintermediate layer 11 comprises a trap-rich layer 111 and a buriedinsulator 121 formed on top of the trap-rich layer 111. The buriedinsulator 121 comprises silicon dioxide and the trap-rich layer 111 comprises silicon. A thickness of the buriedinsulator 121 is between 100nm and 500nm. A thickness of the trap-rich layer 111 can be, for example, several micrometers. According to an alternative embodiment, the buriedinsulator 121 comprises silicon dioxide and the trap-rich layer 111 comprises silicon carbide, for example, amorphous silicon carbide. A thickness of the trap-rich layer 111 can be, for example, tens of nanometers. -
FIG. 3 schematically depicts a cross-section of an example embodiment of asemiconductor structure 1 according to the present disclosure, wherein the cross-section is performed along a plane comprising agrowth direction 2, and atraverse direction 3 traverse to thegrowth direction 2. Athird direction 4 is traverse to thegrowth direction 2 and to thetraverse direction 3. Components having identical reference numbers than onFIG. 2 fulfill the same function. Thesemiconductor structure 1 comprises a Silicon-On-Insulator substrate 101 and an epitaxial III-Nsemiconductor layer stack 202 on top of the Silicon-On-Insulator substrate 101. The Silicon-On-Insulator substrate 101 comprises abase layer 10, anintermediate layer 11 formed on top of thebase layer 10, and atop layer 12 formed on top of theintermediate layer 11. Thebase layer 10 comprises silicon. The resistivity of thebase layer 10 is typically between 3 and 5kOhm·cm, higher than 1 kOhm·cm. The epitaxial III-Nsemiconductor layer stack 202 comprises an epitaxialactive layer 20. The epitaxialactive layer 20 comprises a first active III-N layer 21 formed on top of thetop layer 12 and a second active III-N layer formed on top of the first active III-N layer 21. The first active III-N layer 21 comprises, for example, gallium nitride and the second active III-N layer 22, for example, comprises aluminum gallium nitride. A two-dimensional Electron Gas 200 is formed between the first active III-N layer 21 and the second active III-N layer 22. Thetop layer 12 comprises n-type doped silicon. An orientation of the silicon of thetop layer 12 is (111). The n-type doping concentration of thetop layer 12 is within the range of 1.1015 cm−3 to 5.1015 cm−3. A thickness of thetop layer 12 is between 50 and 200 nm. According to an alternative embodiment, a thickness of thetop layer 12 is lower than 100nm. Theintermediate layer 11 comprises a trap-rich layer 111 and a buriedinsulator 121 formed on top of the trap-rich layer 111. The buriedinsulator 121 comprises alayer 131 comprising silicon nitride confined between twolayers 132; 133 comprising silicon oxide and the trap-rich layer 111 comprises silicon carbide, for example, amorphous silicon carbide. According to an alternative embodiment, the buriedinsulator 121 comprises silicon dioxide and the trap-rich layer 111 comprises silicon carbide, for example, amorphous silicon carbide. A thickness of the buriedinsulator 121 is between 100 nm and 500 nm. A thickness of the trap-rich layer 111 can be, for example, tens of nanometers. According to a further alternative embodiment, the buriedinsulator 121 comprises silicon dioxide and the trap-rich layer 111 comprises silicon. A thickness of the trap-rich layer 111 can be, for example, several micrometers. -
FIG. 4 schematically depicts a cross-section of an example embodiment of asemiconductor structure 1 according to the present disclosure, wherein the cross-section is performed along a plane comprising agrowth direction 2, and atraverse direction 3 traverse to thegrowth direction 2. Athird direction 4 is traverse to thegrowth direction 2 and to thetraverse direction 3. Components having identical reference numbers inFIG. 2 orFIG. 3 fulfill the same function. Thesemiconductor structure 1 comprises a Silicon-On-Insulator substrate 101 and an epitaxial III-Nsemiconductor layer stack 202 on top of the Silicon-On-Insulator substrate 101. The Silicon-On-Insulator substrate 101 comprises abase layer 10, anintermediate layer 11 formed on top of thebase layer 10, and atop layer 12 formed on top of theintermediate layer 11. Thebase layer 10 comprises silicon. The resistivity of thebase layer 10 is typically between 3 and 5 kOhm·cm, higher than 1 kOhm·cm. The epitaxial III-Nsemiconductor layer stack 202 comprises an epitaxialactive layer 20. The epitaxialactive layer 20 comprises a first active III-N layer 21 formed on top of thetop layer 12, aspacer layer 23 formed on top of the first active III-N layer 21, and a second active III-N layer formed on top of thespacer layer 23. The first active III-N layer 21 comprises, for example, gallium nitride and the second active III-N layer 22, for example, comprises aluminum gallium nitride. Thespacer layer 23 preferably comprises aluminum nitride. A two-dimensional Electron Gas 200 is formed between the first active III-N layer 21 and the second active III-N layer 22. Thetop layer 12 comprises n-type doped silicon. An orientation of the silicon of thetop layer 12 is (111). The n-type doping concentration of thetop layer 12 is within the range of 1.1015 cm−3 to 5.1015 cm−3. A thickness of thetop layer 12 is between 50 and 200 nm. According to an alternative embodiment, a thickness of thetop layer 12 is lower than 100 nm. Theintermediate layer 11 comprises a trap-rich layer 111 and a buriedinsulator 121 formed on top of the trap-rich layer 111. The buriedinsulator 121 comprises silicon dioxide and the trap-rich layer 111 comprises silicon. A thickness of the buriedinsulator 121 is between 100 nm and 500 nm. A thickness of the trap-rich layer 111 can be, for example, several micrometers. According to an alternative embodiment, the buriedinsulator 121 comprises silicon dioxide and the trap-rich layer 111 comprises silicon carbide, for example, amorphous silicon carbide. A thickness of the trap-rich layer 111 can be, for example, several micrometers. - Although the present disclosure has been illustrated by reference to specific embodiments, it will be apparent to those skilled in the art that the invention is not limited to the details of the foregoing illustrative embodiments, and that the present disclosure may be embodied with various changes and modifications without departing from the scope thereof. The present embodiments are therefore to be considered in all respects as illustrative and not restrictive, the scope of the invention being indicated by the appended claims rather than by the foregoing description, and all changes that come within the scope of the claims are therefore intended to be embraced therein.
- It will furthermore be understood by the reader of this disclosure that the words “comprising” or “comprise” do not exclude other elements or steps, that the words “a” or “an” do not exclude a plurality, and that a single element, such as a computer system, a processor, or another integrated unit may fulfil the functions of several means recited in the claims. Any reference signs in the claims shall not be construed as limiting the respective claims concerned. The terms “first,” “second,” “third,” “a,” “b,” “c,” and the like, when used in the description or in the claims are introduced to distinguish between similar elements or steps and are not necessarily describing a sequential or chronological order. Similarly, the terms “top,” “bottom,” “over,” “under,” and the like are introduced for descriptive purposes and not necessarily to denote relative positions. It is to be understood that the terms so used are interchangeable under appropriate circumstances and embodiments of the invention can operate according to the present disclosure in other sequences, or in orientations different from the one(s) described or illustrated above.
Claims (15)
Applications Claiming Priority (3)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
FR2113655 | 2021-12-16 | ||
FR2113655A FR3131075B1 (en) | 2021-12-16 | 2021-12-16 | GROUP III NITRIDE SEMICONDUCTOR STRUCTURE ON SILICON ON INSULATION AND ITS GROWTH METHOD |
PCT/EP2022/082085 WO2023110267A1 (en) | 2021-12-16 | 2022-11-16 | Group iii-nitride semiconductor structure on silicon-on-insulator and method of growing thereof |
Publications (1)
Publication Number | Publication Date |
---|---|
US20250056858A1 true US20250056858A1 (en) | 2025-02-13 |
Family
ID=81648394
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
US18/720,416 Pending US20250056858A1 (en) | 2021-12-16 | 2022-11-16 | Group iii-nitride semiconductor structure on silicon-on-insulator and method of growing thereof |
Country Status (8)
Country | Link |
---|---|
US (1) | US20250056858A1 (en) |
EP (1) | EP4449482A1 (en) |
JP (1) | JP2024545586A (en) |
KR (1) | KR20240116563A (en) |
CN (1) | CN118679556A (en) |
FR (1) | FR3131075B1 (en) |
TW (1) | TW202341486A (en) |
WO (1) | WO2023110267A1 (en) |
Family Cites Families (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7999288B2 (en) * | 2007-11-26 | 2011-08-16 | International Rectifier Corporation | High voltage durability III-nitride semiconductor device |
JP5117588B2 (en) * | 2010-09-07 | 2013-01-16 | 株式会社東芝 | Method for manufacturing nitride semiconductor crystal layer |
JP5903818B2 (en) * | 2011-09-26 | 2016-04-13 | 富士通株式会社 | Compound semiconductor device and manufacturing method thereof |
US9721969B2 (en) * | 2015-06-30 | 2017-08-01 | Globalfoundries Singapore Pte. Ltd. | Creation of wide band gap material for integration to SOI thereof |
US10644142B2 (en) * | 2017-12-22 | 2020-05-05 | Nxp Usa, Inc. | Semiconductor devices with doped regions functioning as enhanced resistivity regions or diffusion barriers, and methods of fabrication therefor |
-
2021
- 2021-12-16 FR FR2113655A patent/FR3131075B1/en active Active
-
2022
- 2022-11-16 JP JP2024527762A patent/JP2024545586A/en active Pending
- 2022-11-16 KR KR1020247023870A patent/KR20240116563A/en active Pending
- 2022-11-16 EP EP22817285.4A patent/EP4449482A1/en active Pending
- 2022-11-16 WO PCT/EP2022/082085 patent/WO2023110267A1/en active Application Filing
- 2022-11-16 CN CN202280082217.4A patent/CN118679556A/en active Pending
- 2022-11-16 US US18/720,416 patent/US20250056858A1/en active Pending
- 2022-11-22 TW TW111144574A patent/TW202341486A/en unknown
Also Published As
Publication number | Publication date |
---|---|
FR3131075B1 (en) | 2023-12-22 |
FR3131075A1 (en) | 2023-06-23 |
CN118679556A (en) | 2024-09-20 |
EP4449482A1 (en) | 2024-10-23 |
WO2023110267A1 (en) | 2023-06-22 |
TW202341486A (en) | 2023-10-16 |
JP2024545586A (en) | 2024-12-10 |
KR20240116563A (en) | 2024-07-29 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US9831312B2 (en) | Group III-V device structure having a selectively reduced impurity concentration | |
US9130026B2 (en) | Crystalline layer for passivation of III-N surface | |
CN103201840B (en) | HEMTs with improved buffer breakdown voltage | |
US20080070355A1 (en) | Aspect ratio trapping for mixed signal applications | |
US8242001B2 (en) | Apparatus and methods for improving parallel conduction in a quantum well device | |
US8558285B2 (en) | Method using low temperature wafer bonding to fabricate transistors with heterojunctions of Si(Ge) to III-N materials | |
US20150349124A1 (en) | Transistor structure having buried island regions | |
US20160380104A1 (en) | Iii-v gate-all-around field effect transistor using aspect ratio trapping | |
US10074734B2 (en) | Germanium lateral bipolar transistor with silicon passivation | |
US20170222048A1 (en) | Implementation of long-channel thick-oxide devices in vertical transistor flow | |
US20160268134A1 (en) | Method for manufacturing semiconductor device | |
US20250056858A1 (en) | Group iii-nitride semiconductor structure on silicon-on-insulator and method of growing thereof | |
JP6531243B2 (en) | Tunnel field effect transistor and method of manufacturing field effect transistor | |
US9437675B1 (en) | eDRAM for planar III-V semiconductor devices | |
EP4117041A1 (en) | Semiconductor structure with barrier layer comprising indium aluminium nitride and method of growing thereof | |
US11784189B2 (en) | Monolithic integration of diverse device types with shared electrical isolation | |
WO2023194211A1 (en) | High electron mobility transistor and method of manufacturing thereof |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
AS | Assignment |
Owner name: SOITEC BELGIUM, BELGIUM Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:VEYTIZOU, CHRYSTELLE;RADU, IONUT;DERLUYN, JOFF;AND OTHERS;SIGNING DATES FROM 20240523 TO 20240723;REEL/FRAME:068500/0852 Owner name: SOITEC, FRANCE Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:VEYTIZOU, CHRYSTELLE;RADU, IONUT;DERLUYN, JOFF;AND OTHERS;SIGNING DATES FROM 20240523 TO 20240723;REEL/FRAME:068500/0852 |
|
AS | Assignment |
Owner name: SOITEC BELGIUM, BELGIUM Free format text: CORRECTIVE ASSIGNMENT TO CORRECT THE CORRECT THE SPELLING OF THE FIRST NAMED INVENTOR'S NAME PREVIOUSLY RECORDED AT REEL: 68500 FRAME: 852. ASSIGNOR(S) HEREBY CONFIRMS THE ASSIGNMENT;ASSIGNORS:VEYTIZOU, CHRISTELLE;RADU, IONUT;DERLUYN, JOFF;AND OTHERS;SIGNING DATES FROM 20240523 TO 20240723;REEL/FRAME:069167/0974 |
|
STPP | Information on status: patent application and granting procedure in general |
Free format text: DOCKETED NEW CASE - READY FOR EXAMINATION |